Papers by Author: Chong Qing Huang

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Abstract: The ferroelectricity of Bi3.25Sm0.75Ti3O12 (BST), and Bi3.25Sm0.75Ti2.97V0.03O12 (BSTV) ceramics prepared at 1100°C by a conventional ceramic technique was investigated. These ceramics possess random-oriented polycrystalline structure. The remanent polarization (Pr) and coercive field (Ec) of the BST ceramics are 16 µC/cm2 and 64kV/cm, respectively. Furthermore, V substitution improves the Pr value of the BST ceramics up to 25 μC/cm2, which is much larger than that of the BST ceramics. Therefore, co-sustitution of Sm and V in is effective for the improvement of the ferroelectricity of Bi4Ti3O12 ceramic.
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Abstract: The electrical properties of Tb4O7-bismuth titanate (Bi3.3Tb0.6Ti3O12) prepared by a conventional ceramic technique have been investigated. At applied d.c. field below 200V/mm, the current-voltage curve of Tb-doped sample exhibits a simple ohmic behavior. The impedance spectrum of Tb-doped sample indicates that consist of semiconducting grain and moderately insulating grain boundary regions. XRD, SEM and EPMA analyses reveal crystalline phase characterized by a Bi-layered perovskite structure of Bi4Ti3O12 and the distribution of every element is uniform. Tb-doped sample exhibit randomly oriented and plate-like morphology.
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Abstract: The electrical properties of Pr6O11-doped bismuth titanates (BixPryTi3O12, BPT) ceramics prepared by a conventional ceramic technique have been investigated. At applied d.c. field below 200V/mm, the current-voltage curve of Pr-doped samples exhibit negative differential resistance behavior. The conducting filamentary model has been used to explain the negative differential resistance phenomenon in Pr-doped bismuth titanates. The impedance spectrum indicates that Pr-doped sample consists of semiconducting grain and moderately insulating grain boundary regions. XRD, SEM and EPMA analyses reveal crystalline phase characterized by a Bi-layered perovskite structure of Bi4Ti3O12 and the distribution of every element is uniform. Pr-doped samples exhibit randomly oriented and plate-like morphology.
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Abstract: The electrical properties of Gd-doped bismuth titanates Bi4-xGdxTi3O12) prepared by a conventional ceramic technique have been investigated. At applied d.c. field below 200V/mm, the current-voltage curve of Gd-doped sample exhibits a negative differential resistance behavior. The conducting filamentary model has been used to explain the negative differential resistance phenomenon in Gd-doped bismuth titanates. The impedance spectrum of Gd sample indicates that both consist of semiconducting grain and moderately insulating grain boundary regions. XRD, SEM and EPMA analyses reveal crystalline phase characterized by a Bi-layered perovskite structure of Bi4Ti3O12 and the distribution of every element is uniform. Gd-doped sample exhibites randomly oriented and plate-like morphology.
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Abstract: Bi3.25La0.75Ti2.97V0.03O12 (BLTV) ceramic were prepared by solid state reaction. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed plate-like grains with random orientation. BLTV caused a large shift of the Curie temperature ( TC ) of Bi4Ti3O12 (BIT) from 675°C to 395°C. The remanent polarization and the coercive field of the BLTV were 31μC/cm2 and 54kV/cm at an electric field of 90kV/cm, respectively. Furthermore, the dielectric permittivity and dissipation factor were 300 and 3×10-3 at 1MHz, at 1V and at room temperature, respectively. These ferroelectric properties of BLTV are superior to V-doped Bi4Ti3O12 (~20μC/cm2 and 80kV/cm) and (Sr, Ta)-doped Bi4Ti3O12 (~12μC/cm2 and 71kV/cm) ceramics. In addition, the dense ceramics of BLTV could be obtained by sintering at temperatures 100─200°C lower than those of the SrBi2Ta2O9 system.
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Abstract: The ferroelectricity of Bi3.25Dy0.75Ti3O12 (BDT), and Bi3.25Dy0.75Ti2.97V0.03O12 (BDTV) ceramics prepared at 1100°C by a conventional ceramic technique was investigated. These ceramics possess random-oriented polycrystalline structure. The remanent polarization (Pr) and coercive field (Ec) of the BDT ceramics are 15 µC/cm2 and 64kV/cm, respectively. Furthermore, V substitution improves the Pr value of the BDT ceramics up to 23 μC/cm2, which is much larger than that of the BDT ceramics. Therefore, co-sustitution of D and V in Bi4Ti3O12 (BIT) ceramic is effective for the improvement of its ferroelectricity.
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Abstract: The electrical properties of La-doped bismuth titanate, Bi4-xLaxTi3O12 (BLT) ceramics prepared by a conventional electroceramic technique have been investigated. XRD analyses revealed Bi-layered perovskite structure in all samples, and indicted that Bi ions were only substituted near the Ti-O octahedron layers by La ions. SEM micrographs show randomly oriented and plate-like morphology. The remanent polarization ( Pr ) and coercive field ( Ec ) of the BLT ceramic with x=0.75 were above 19μC/cm2 and 60KV/cm, respectively. The large value of remanent polarization and low coercive field of La-doped bismuth titanate ceramics promote these materials to potential applications.
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Abstract: The electrical properties of Ce-doped bismuth titanate, Bi4-xCexTi3O12 (BCT) ceramics prepared by a conventional electroceramic technique were investigated. XRD analyses revealed Bi-layered perovskite structure in all samples. SEM micrographs showed randomly oriented and plate-like morphology. For the samples with x=0.4 and 1.0 the current-voltage characteristics exhibited negative differential resistance behaviors and their P-E hysteresis loops were characterized by large leakage current, whereas for the samples with x=0.6 and 0.8 the current-voltage characteristics showed simple ohmic behaviors and their P-E hysteresis loops were the saturated and undistorted hysteresis loops. The remanent polarization ( Pr ) and coercive field (Ec) of the BCT ceramic with x=0.8 were above 20μC/cm2 and 60KV/cm , respectively.
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Abstract: Eu2O3-doped bismuth titanate (Bi4-xEuxTi3O12: BET) thin films with random oriention were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique, and the structures and ferroelectric properties of the films were investigated. XRD studies indicated that all of BET films consisted of single phase of a bismuth-layered structure with well-developed rod-like grains. The remanent polarization ( Pr ) and coercive field (Ec) of the BET Film with x=0.8 were 20μC/cm2 and 65KV/cm , respectively. After 3×1010 switching cycles, 15% degradation of Pr is observed in the film.
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Abstract: Bi2WTi3O12 ceramics are fabricated by conventional solid-state reaction process. XRD analysis reveals that Bi2WO6 is the main phase and Bi4Ti3O12 is the second phase. With increasing temperature the sample first appears metallic behavior, then strong electrical fluctuations above 100°C, and finally exhibits stable nonlinear properties characterized by semiconductivity above 300°C at low field (E ≤ 100V/mm). The Arrhenius law for electrical conductivity by thermal activation is not suitable to explain the anomalous results. Based on the phase transition of tungsten trioxide from room temperature to about 300°C, the electrical properties of Bi2WTi3O12 ceramics can be explained.
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